Ribosome Elongation Kinetics of Consecutively Charged Residues Are Coupled to Electrostatic Force.

The speed of protein synthesis can dramatically change when consecutively charged residues are incorporated into an elongating nascent protein by the ribosome. The molecular origins of this class of allosteric coupling remain unknown. We demonstrate, using multiscale simulations, that positively charged residues generate large forces that move the P-site amino acid away from the A-site amino acid. Negatively charged residues generate forces of similar magnitude but move the A- and P-sites closer together. These conformational changes, respectively, increase and decrease the transition state barrier height to peptide bond formation, explaining how charged residues mechanochemically alter translation speed. This mechanochemical mechanism is consistent with in vivo ribosome profiling data exhibiting proportionality between translation speed and the number of charged residues, experimental data characterizing nascent chain conformations, and a previously published cryo-EM structure of a ribosome-nascent chain complex containing consecutive lysines. These results expand the role of mechanochemistry in translation and provide a framework for interpreting experimental results on translation speed.

Forcing the ribosome to change its message.

Mechanical forces can be generated when nascent protein segments are integrated into a membrane. These forces are then transmitted through the nascent protein to the ribosome's catalytic core, but only a few biological consequences of this process have been identified to date. In this issue, Harrington et al. present evidence that these forces form a conserved mechanism to influence the efficiency of ribosomal frameshifting during translation of viral RNA, indicating that mechanical forces may play a broader regulatory role in translation than previously appreciated.

Side-chain thioamides as fluorescence quenching probes.

Thioamides, single atom oxygen-to-sulfur substitutions of canonical amide bonds, can be valuable probes for protein folding and protease studies. Here, we investigate the fluorescence quenching properties of thioamides incorporated into the side-chains of amino acids. We synthesize and incorporate Fmoc-protected, solid-phase peptide synthesis building blocks for introducing Nε -thioacetyl-lysine and γ-thioasparagine. Using rigid model peptides, we demonstrate the distance-dependent fluorescence quenching of these thioamides. Furthermore, we describe attempts to incorporate of Nε -thioacetyl-lysine into proteins expressed in Escherichia coli using amber codon suppression.

Mechanochemistry in Translation.

As the influence of translation rates on protein folding and function has come to light, the mechanisms by which translation speed is modulated have become an important issue. One mechanism entails the generation of force by the nascent protein. Cotranslational processes, such as nascent protein folding, the emergence of unfolded nascent chain segments from the ribosome's exit tunnel, and insertion of the nascent chain into or translocation of the nascent chain through membranes, can generate forces that are transmitted back to the peptidyl transferase center and affect translation rates. In this Perspective, we examine the processes that generate these forces, the mechanisms of transmission along the ribosomal exit tunnel to the peptidyl transferase center, and the effects of force on the ribosome's catalytic cycle. We also discuss the physical models that have been developed to predict and explain force generation for individual processes and speculate about other processes that may generate forces that have yet to be tested.

Origins of the Mechanochemical Coupling of Peptide Bond Formation to Protein Synthesis.

Mechanical forces acting on the ribosome can alter the speed of protein synthesis, indicating that mechanochemistry can contribute to translation control of gene expression. The naturally occurring sources of these mechanical forces, the mechanism by which they are transmitted 10 nm to the ribosome's catalytic core, and how they influence peptide bond formation rates are largely unknown. Here, we identify a new source of mechanical force acting on the ribosome by using in situ experimental measurements of changes in nascent-chain extension in the exit tunnel in conjunction with all-atom and coarse-grained computer simulations. We demonstrate that when the number of residues composing a nascent chain increases, its unstructured segments outside the ribosome exit tunnel generate piconewtons of force that are fully transmitted to the ribosome's P-site. The route of force transmission is shown to be through the nascent polypetide's backbone, not through the wall of the ribosome's exit tunnel. Utilizing quantum mechanical calculations we find that a consequence of such a pulling force is to decrease the transition state free energy barrier to peptide bond formation, indicating that the elongation of a nascent chain can accelerate translation. Since nascent protein segments can start out as largely unfolded structural ensembles, these results suggest a pulling force is present during protein synthesis that can modulate translation speed. The mechanism of force transmission we have identified and its consequences for peptide bond formation should be relevant regardless of the source of the pulling force.

Determinants of pore folding in potassium channel biogenesis.

Many ion channels, both selective and nonselective, have reentrant pore loops that contribute to the architecture of the permeation pathway. It is a fundamental feature of these diverse channels, regardless of whether they are gated by changes of membrane potential or by neurotransmitters, and is critical to function of the channel. Misfolding of the pore loop leads to loss of trafficking and expression of these channels on the cell surface. Mature tetrameric potassium channels contain an α-helix within the pore loop. We systematically mutated the "pore helix" residues of the channel Kv1.3 and assessed the ability of the monomer to fold into a tertiary reentrant loop. Our results show that pore loop residues form a canonical α-helix in the monomer early in biogenesis and that disruption of tertiary folding is caused by hydrophilic substitutions only along one face of this α-helix. These results provide insight into the determinants of the reentrant pore conformation, which is essential for ion channel function.

Biogenesis of the pore architecture of a voltage-gated potassium channel.

The pore domain of voltage-gated potassium (Kv) channels consists of transmembrane helices S5 and S6, the turret, the pore helix, the selectivity filter, and the loop preceding S6, with a tertiary reentrant structure between S5 and S6. Using biogenic intermediates, mass tagging (pegylation), and a molecular tape measure, we explored the possibility that the first stages of pore formation occur prior to oligomerization of the transmembrane core. Pegylation of introduced cysteines shows that the pore helix, but not the turret, forms a compact secondary structure in the terminal 20 Å of the ribosomal tunnel. We assessed the tertiary fold of the pore loop in monomeric constructs by determining the relative accessibilities of select cysteines using the kinetics of pegylation. Turret residues are accessible at the extracellular surface. In contrast, pore helix residues are less accessible. All-atom molecular dynamics simulations of a single Kv monomer in a solvated lipid membrane indicate that secondary and tertiary folds are stable over 650 ns. These results are consistent with acquisition of a tertiary reentrant pore architecture at the monomer stage of Kv biogenesis and begin to define a plausible sequence of folding events in the formation of Kv channels.

Molecular rearrangements in S6 during slow inactivation in Shaker-IR potassium channels.

Voltage-gated K+ channels have distinct gates that regulate ion flux: the activation gate (A-gate) formed by the bundle crossing of the S6 transmembrane helices and the slow inactivation gate in the selectivity filter. These two gates are bidirectionally coupled. If coupling involves the rearrangement of the S6 transmembrane segment, then we predict state-dependent changes in the accessibility of S6 residues from the water-filled cavity of the channel with gating. To test this, we engineered cysteines, one at a time, at S6 positions A471, L472, and P473 in a T449A Shaker-IR background and determined the accessibility of these cysteines to cysteine-modifying reagents MTSET and MTSEA applied to the cytosolic surface of inside-out patches. We found that neither reagent modified either of the cysteines in the closed or the open state of the channels. On the contrary, A471C and P473C, but not L472C, were modified by MTSEA, but not by MTSET, if applied to inactivated channels with open A-gate (OI state). Our results, combined with earlier studies reporting reduced accessibility of residues I470C and V474C in the inactivated state, strongly suggest that the coupling between the A-gate and the slow inactivation gate is mediated by rearrangements in the S6 segment. The S6 rearrangements are consistent with a rigid rod-like rotation of S6 around its longitudinal axis upon inactivation. S6 rotation and changes in its environment are concomitant events in slow inactivation of Shaker KV channels.

Folding zones inside the ribosomal exit tunnel.

Helicity of membrane proteins can be manifested inside the ribosome tunnel, but the determinants of compact structure formation inside the tunnel are largely unexplored. Using an extended nascent peptide as a molecular tape measure of the ribosomal tunnel, we have previously demonstrated helix formation inside the tunnel. Here, we introduce a series of consecutive polyalanines into different regions of the tape measure to monitor the formation of compact structure in the nascent peptide. We find that the formation of compact structure of the polyalanine sequence depends on its location. Calculation of free energies for the equilibria between folded and unfolded nascent peptides in different regions of the tunnel shows that there are zones of secondary structure formation inside the ribosomal exit tunnel. These zones may have an active role in nascent-chain compaction.

The activation gate controls steady-state inactivation and recovery from inactivation in Shaker.

Despite major advances in the structure determination of ion channels, the sequence of molecular rearrangements at negative membrane potentials in voltage-gated potassium channels of the Shaker family remains unknown. Four major composite gating states are documented during the gating process: closed (C), open (O), open-inactivated (OI), and closed-inactivated (CI). Although many steps in the gating cycle have been clarified experimentally, the development of steady-state inactivation at negative membrane potentials and mandatory gating transitions for recovery from inactivation have not been elucidated. In this study, we exploit the biophysical properties of Shaker-IR mutants T449A/V474C and T449A/V476C to evaluate the status of the activation and inactivation gates during steady-state inactivation and upon locking the channel open with intracellular Cd2+. We conclude that at negative membrane potentials, the gating scheme of Shaker channels can be refined in two aspects. First, the most likely pathway for the development of steady-state inactivation is C→O→OI⇌CI. Second, the OI→CI transition is a prerequisite for recovery from inactivation. These findings are in accordance with the widely accepted view that tight coupling is present between the activation and C-type inactivation gates in Shaker and underscore the role of steady-state inactivation and recovery from inactivation as determinants of excitability.

Coupled tertiary folding and oligomerization of the T1 domain of Kv channels.

Acquisition of secondary, tertiary, and quaternary structure is critical to the fabrication, assembly, and function of ion channels, yet the relationship between these biogenic events remains unclear. We now address this issue in voltage-gated K(+) channels (Kv) for the T1 domain, an N-terminal Kv recognition domain that is responsible for subfamily-specific, efficient assembly of Kv subunits. This domain forms a 4-fold symmetric tetramer. We have identified residues along the axial T1-T1 interface that are critical for tertiary and quaternary structure, shown that mutations at one end of the axial T1 interface can perturb the crosslinking of an intersubunit cysteine pair at the other end, and demonstrated that tertiary folding and tetramerization of this Kv domain are coupled. A threshold level of tertiary folding is required for monomers to oligomerize. Coupling between tertiary and quaternary structure formation may be a common feature in the biogenesis of multimeric proteins.

The birth of a channel.

An ion channel protein begins life as a nascent peptide inside a ribosome, moves to the endoplasmic reticulum where it becomes integrated into the lipid bilayer, and ultimately forms a functional unit that conducts ions in a well-regulated fashion. Here, I discuss the nascent peptide and its tasks as it wends its way through ribosomal tunnels and exit ports, through translocons, and into the bilayer. We are just beginning to explore the sequence of these events, mechanisms of ion channel structure formation, when biogenic decisions are made, and by which participants. These decisions include when to exit the endoplasmic reticulum and with whom to associate. Such issues govern the expression of ion channels at the cell surface and thus the electrical activity of a cell.

Structure acquisition of the T1 domain of Kv1.3 during biogenesis.

The T1 recognition domains of voltage-gated K(+) (Kv) channel subunits form tetramers and acquire tertiary structure while still attached to their individual ribosomes. Here we ask when and in which compartment secondary and tertiary structures are acquired. We answer this question using biogenic intermediates and recently developed folding and accessibility assays to evaluate the status of the nascent Kv peptide both inside and outside of the ribosome. A compact structure (likely helical) that corresponds to a region of helicity in the mature structure is already manifest in the nascent protein within the ribosomal tunnel. The T1 domain acquires tertiary structure only after emerging from the ribosomal exit tunnel and complete synthesis of the T1-S1 linker. These measurements of ion channel folding within the ribosomal tunnel and its exit port bear on basic principles of protein folding and pave the way for understanding the molecular basis of protein misfolding, a fundamental cause of channelopathies.

Probing the cavity of the slow inactivated conformation of shaker potassium channels.

Slow inactivation involves a local rearrangement of the outer mouth of voltage-gated potassium channels, but nothing is known regarding rearrangements in the cavity between the activation gate and the selectivity filter. We now report that the cavity undergoes a conformational change in the slow-inactivated state. This change is manifest as altered accessibility of residues facing the aqueous cavity and as a marked decrease in the affinity of tetraethylammonium for its internal binding site. These findings have implications for global alterations of the channel during slow inactivation and putative coupling between activation and slow-inactivation gates.

Mapping the electrostatic potential within the ribosomal exit tunnel.

Electrostatic potentials influence interactions among proteins and nucleic acids, the orientation of dipoles and quadrupoles, and the distribution of mobile charges. Consequently, electrostatic potentials can modulate macromolecular folding and conformational stability, as well as rates of catalysis and substrate binding. The ribosomal exit tunnel, along with its resident nascent peptide, is no less susceptible to these consequences. Yet, the electrostatics inside the tunnel have never been measured. Here we map both the electrostatic potential and accessibilities along the length of the tunnel and determine the electrostatic consequences of introducing a charged amino acid into the nascent peptide. To do this we developed novel probes and strategies. Our findings provide new insights regarding the dielectric of the tunnel and the dynamics of its local electric fields.

Cross talk between activation and slow inactivation gates of Shaker potassium channels.

This study addresses the energetic coupling between the activation and slow inactivation gates of Shaker potassium channels. To track the status of the activation gate in inactivated channels that are nonconducting, we used two functional assays: the accessibility of a cysteine residue engineered into the protein lining the pore cavity (V474C) and the liberation by depolarization of a Cs(+) ion trapped behind the closed activation gate. We determined that the rate of activation gate movement depends on the state of the inactivation gate. A closed inactivation gate favors faster opening and slower closing of the activation gate. We also show that hyperpolarization closes the activation gate long before a channel recovers from inactivation. Because activation and slow inactivation are ubiquitous gating processes in potassium channels, the cross talk between them is likely to be a fundamental factor in controlling ion flux across membranes.

A trapped intracellular cation modulates K+ channel recovery from slow inactivation.

Upon depolarization, many voltage-gated potassium channels undergo a time-dependent decrease in conductance known as inactivation. Both entry of channels into an inactivated state and recovery from this state govern cellular excitability. In this study, we show that recovery from slow inactivation is regulated by intracellular permeant cations. When inactivated channels are hyperpolarized, closure of the activation gate traps a cation between the activation and inactivation gates. The identity of the trapped cation determines the rate of recovery, and the ability of cations to promote recovery follows the rank order K+ > NH4+ > Rb+ > Cs+ >> Na+, TMA. The striking similarity between this rank order and that for single channel conductance suggests that these two processes share a common feature. We propose that the rate of recovery from slow inactivation is determined by the ability of entrapped cations to move into a binding site in the channel's selectivity filter, and refilling of this site is required for recovery.

Determinants of Helix Formation for a Kv1.3 Transmembrane Segment inside the Ribosome Exit Tunnel.

Proteins begin to fold in the ribosome, and misfolding has pathological consequences. Among the earliest folding events in biogenesis is the formation of a helix, an elementary structure that is ubiquitously present and required for correct protein folding in all proteomes. The determinants underlying helix formation in the confined space of the ribosome exit tunnel are relatively unknown. We chose the second transmembrane segment, S2, of a voltage-gated potassium channel, Kv1.3, as a model to probe this issue. Since the N terminus of S2 is initially in an extended conformation in the folding vestibule of the ribosome yet ultimately emerges at the exit port as a helix, S2 is ideally suited for delineating sequential events and folding determinants of helix formation inside the ribosome. We show that S2's extended N terminus inside the tunnel is converted into a helix by a single, distant mutation in the nascent peptide. This transition depends on nascent peptide sequence at specific tunnel locations. Co-translational secondary folding of nascent chains inside the ribosome has profound physiological consequences that bear on correct membrane insertion, tertiary folding, oligomerization, and biochemical modification of the newborn protein during biogenesis.

Effect of Nascent Peptide Steric Bulk on Elongation Kinetics in the Ribosome Exit Tunnel.

All proteins are synthesized by the ribosome, a macromolecular complex that accomplishes the life-sustaining tasks of faithfully decoding mRNA and catalyzing peptide bond formation at the peptidyl transferase center (PTC). The ribosome has evolved an exit tunnel to host the elongating new peptide, protect it from proteolytic digestion, and guide its emergence. It is here that the nascent chain begins to fold. This folding process depends on the rate of translation at the PTC. We report here that besides PTC events, translation kinetics depend on steric constraints on nascent peptide side chains and that confined movements of cramped side chains within and through the tunnel fine-tune elongation rates.